By using lattice QCD computations we determine the sigma terms and strangeness content of all octet baryons by means of an application of the Hellmann-Feynman theorem. In addition to polynomial and rational expressions for the quark-mass dependence of octet members, we use $SU(3)$ covariant baryon chiral perturbation theory to perform the extrapolation to the physical up and down quark masses. Our Nf=2+1 lattice ensembles include pion masses down to about 190 MeV in large volumes (M_πL4), and three values of the lattice spacing. Our main results are the nucleon sigma term σ_πN=39(4)(_-7⁺¹⁸) and the strangeness content yN=0.20(7)(_-17⁺¹³). Under the assumption of validity of covariant baryon χPT in our range of masses one finds yN=0.276(77)(_-62⁺⁹⁰).
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Dürr et al. (2012) studied this question.
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